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A Review of Nonimaging Solar Concentrators for Stationary and Passive Tracking Applications ⁎ Srikanth Madala , Robert F

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A Review of Nonimaging Solar Concentrators for Stationary and Passive Tracking Applications ⁎ Srikanth Madala , Robert F Renewable and Sustainable Energy Reviews (xxxx) xxxx–xxxx Contents lists available at ScienceDirect Renewable and Sustainable Energy Reviews journal homepage: www.elsevier.com/locate/rser A review of nonimaging solar concentrators for stationary and passive tracking applications ⁎ Srikanth Madala , Robert F. Boehm Center for Energy Research, Department of Mechanical Engineering, University of Nevada, Las Vegas 89154-4027, United States ARTICLE INFO ABSTRACT Keywords: The solar energy research community has realized the redundancy of image-forming while collecting/ Solar concentrators concentrating solar energy with the discovery of the nonimaging type radiation collection mechanism in Nonimaging optics 1965. Since then, various nonimaging concentration mechanisms have proven their superior collection CPC efficiency over their imaging counter-parts. The feasibility of using nonimaging concentrators successfully for Compound parabolic concentrator stationary applications has rekindled interest in them. The economic benefits are appealing owing to the V-trough elimination of tracking costs (installation, operation & maintenance and auxiliary energy). This paper is an Polygonal trough Concentration ratio exhaustive review of the available nonimaging concentrating mechanisms with stationary applications in mind. Non-tracking solar concentrators This paper also explores the idea of coupling nonimaging concentrators with passive solar tracking mechanism. Stationary solar concentrators CHC CEC Compound hyperbolic concentrators Compound elliptical concentrators Nonimaging Fresnel lenses Dielectric compound parabolic concentrators DCPC Trumpet-shaped concentrators 1. Introduction traditional imaging techniques of concentration fall short of the thermodynamic limit of maximum attainable concentration at least Amongst the total solar electric power worldwide today (as per by a factor of four due to severe off-axis aberration and coma causing 2015 data) [1], solar photovoltaics (PV) contribute about 227 GW, and image blurring and broadening. Imaging is an inhibitive phenomenon concentrating solar power (CSP) technologies contribute about 4.8 GW as far as only energy concentration is concerned. The concentration of in generation capacity. NREL's SolarPACES program constantly moni- solar energy does not demand imaging qualities, but instead requires tors and updates the global list of CSP projects that are either flexible concentrator designs coping with solar disk size, solar spec- operational or currently under development [2]. The parabolic trough trum, and tracking errors while delivering a highly uniform flux [4]. (an imaging-type solar concentrator technology) accounts for a vast Moreover, an active solar tracking mechanism, often accompanying an majority of the CSP installations worldwide due to its cost advantage, imaging concentrator, also adds to the capital and O & M costs while although power tower systems are quickly catching up. United States consuming a fraction of the power produced. Therefore, with all these and Spain being the front-runners, various other nations including the disadvantages in view, nonimaging and stationary techniques of Middle East and North Africa (MENA) countries, South Africa, India, concentrating solar radiation are sought after. and China are fast adopting CSP [3]. Nonimaging concentrators have been used in solar energy collec- No matter the type of CSP technology adopted, actively tracking the tion systems ever since their discovery in 1965. In the decades that Sun in order to achieve meaningful concentration is a common trait in followed, various nonimaging concentrator designs were discovered all of them. The concentration of solar radiation is typically achieved by and evaluated as stationary installations. The concentration ratios using an active solar tracking mechanism coupled with a point- or line- achieved were typical low ( < 3X) or medium (3-10X). However, the focus imaging concentration system. However, even the best of the application of these types of concentrators on a large scale or a utility ⁎ Corresponding author. E-mail address: [email protected] (S. Madala). http://dx.doi.org/10.1016/j.rser.2016.12.058 Received 6 February 2016; Received in revised form 14 November 2016; Accepted 8 December 2016 1364-0321/ © 2016 Elsevier Ltd. All rights reserved. Please cite this article as: Madala, S., Renewable and Sustainable Energy Reviews (2016), http://dx.doi.org/10.1016/j.rser.2016.12.058 S. Madala, R.F. Boehm Renewable and Sustainable Energy Reviews (xxxx) xxxx–xxxx Nomenclature hcd Conductive Heat Transfer Coefficient hR Radiative Heat Transfer Coefficient CPC Compound Parabolic Concentrator htot Overall Heat Transfer Coefficient ACPC Asymmetric Compound Parabolic Concentrator Htrunc Height of the truncated CPC BIPV Building Integrated Photovoltaics LVT Lens-V Trough CCAC Compound Circular Arc Concentrator MENA Middle East and North Africa CEC Compound Elliptical Concentrator n Refractive Index of the Dielectric Media CHC Compound Hyperbolic Concentrator NREL National Renewable Energy Laboratory CPV Concentrated Photovoltaics O&M Operation and Maintenance CR Concentration Ratio PCCPC Prism-coupled Compound Parabolic Concentrator CSP Concentrated Solar Power PV Photovoltaics CSP Concentrated Solar Power RReflector-To-Aperture Ratio d1 Dimension of Entrance Aperture SPC Simple Parabolic Concentrator d2 Dimension of Exit Aperture α Absorptivity DACPC Dielectric Asymmetric Parabolic Concentrator β Prism Apex Angle DCPC Dielectric Compound Parabolic Concentrator δ Complete Acceptance Angle of V-trough ER Energy Ratio ε Emissivity F(θ) Angular Acceptance Function θ Angle of Incidence of an Arbitrary Light Ray FDTD Finite-Difference Time-Domain θaor θmax Acceptance Angle GW Giga Watt θd Truncated CPC's Edge Ray Angle H Height of the CPC Φ Half Angle Of The V-Shaped Cone hc Convective Heat Transfer Coefficient scale is yet to be materialized. This current paper is a review of the form an image of the light source. Unlike the conventional imaging presently existing and upcoming nonimaging techniques for concen- concentration systems, the quality of the image at the exit aperture is of tration of solar radiation in stationary or passive tracking applications. least importance in these concentrators. An illustration of a hypothe- Novel applications, and modern techniques of raytracing analysis on tical nonimaging concentration system is shown in Fig. 1. The concept nonimaging concentrators has also been discussed as a part of this of nonimaging collection of radiation came into the picture when the review. compound parabolic concentrator (CPC) was proposed by Hinterberg and Winston in 1965 as an efficient means of measuring Čerenkov 2. Stationary solar energy collectors radiation. The early 70 s saw a tremendous rise in the number of researchers experimenting on application of various CPC/modified Stationary solar energy collector designs such as a flat plate and a CPC designs as solar concentrators. All these nonimaging collector concentric cylindrical tube have been prevalent in low temperature ( < designs obey a fundamental principle known as the edge-ray principle 200° F) applications such as solar domestic/pool water heating, (used in the design of nonimaging optics) which can be summed up as: “ dehydration of agricultural products, etc. since the beginning of the if the edge or boundary rays from a source to an optical system fl 20th century [5]. As early as the mid-1970s, Falbel Energy System (re ective or refractive) are able to be directed to the edges of a target Corp. manufactured a stationary ‘nonimaging’ collector (called the FES area, then all the rays in between these edge rays will also be directed to ” delta solar collector) with a cylindrical cavity trough that achieved a net the target area . Winston et al. [8] demonstrated the edge-ray principle fi gain of 2.3X compared to a flat plate collector. Another company using the string method. The same principle has also been re ned by named Kaptron manufactured a modified stationary flat-plate solar using a topological approach [9]. collector by incorporating a window with optical ribs, an optical valve The properties of various nonimaging CPC-type concentrators and a multi-reflection absorber enclosed in an insulated casing, thus including the compound elliptical concentrator (CEC), compound making it more efficient over a conventional design [6]. In more recent hyperbolic concentrator (CHC), trumpet-shaped concentrator and fl times, a Stationary V-trough collector (cone angle=60°) was fabricated generalized involute re ectors were discussed by Gordon and Rabl fl and tested in a solar water heating application for the geographical [10]. A comparative review on various re ective type solar concen- location of Kuala Lumpur (3.2°N and 101° 44′ E) [7]. The collector was trators has been reported as well [11]. Collector characteristics such as oriented in the E-W direction with 0° tilt angle. With a surface area of geometric concentration ratio, acceptance angle, sensitivity to mirror 0.56 m2, it achieved a diurnal power collection that varied between 0.154 and 0.261 kW. When compared with respect to a flat-plate absorber, the average relative solar concentration ratios of the V-trough varied between 1.19 and 1.85 throughout the year. Interestingly, the peak summer and winter months saw a decrement in the relative concentration ratio. 3. Nonimaging solar concentrators Nonimaging concentrators are a classification of radiation collec- tors that direct the
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